/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 20 The given equation is an implici... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

The given equation is an implicit solution of \(N(t, y) y^{\prime}+M(t, y)=0\), satisfying the given initial condition. Assuming the equation \(N(t, y) y^{\prime}+M(t, y)=0\) is exact, determine the functions \(M(t, y)\) and \(N(t, y)\), as well as the possible value(s) of \(y_{0}\). \(y^{3}+4 t y+t^{4}+1=0, \quad y(0)=y_{0}\)

Short Answer

Expert verified
Answer: The functions M(t, y) and N(t, y) are \(M(t, y) = 4y + 4t^3\) and \(N(t, y) = 3y^2 + 4t\), and the possible value of \(y_0\) is \(-1\).

Step by step solution

01

Differentiate the implicit solution with respect to t

Starting with the given implicit solution equation, differentiate it with respect to \(t\). Apply the chain rule when differentiating terms containing \(y(t)\): \[\frac{d}{dt}(y^3 + 4ty + t^4 + 1) = \frac{d}{dt}(0)\] Now, differentiate each term on the left-hand side: \[\frac{d}{dt}(y^3) + \frac{d}{dt}(4ty) + \frac{d}{dt}(t^4) + \frac{d}{dt}(1) = 0\]
02

Find y' term in the derivative

Using the chain rule and product rule, we find the terms involving \(y'\): \[3y^2y' + 4y + 4ty' + 4t^3 = 0\] Now, we can rewrite this equation in the form of \(N(t, y) y^{\prime}+M(t, y)=0\): \[(3y^2 + 4t)y' + (4y + 4t^3) = 0\] Thus, we found the functions \(N(t, y) = 3y^2 + 4t\) and \(M(t, y) = 4y + 4t^3\).
03

Find possible value(s) of \(y_{0}\)

Now let's find the value(s) of \(y_{0}\) for the given initial condition, \(y(0)=y_{0}\). Substitute \(y=y_0\) and \(t=0\) into the given implicit equation: \[y_0^3 + 4(0)(y_0) + 0^4 + 1 = 0\] Solve for \(y_0\): \[y_0^3 + 1 = 0\] \[y_0^3 = -1\] This implies that \(y_0 = \sqrt[3]{-1} = -1\). So, the functions \(M(t, y) = 4y + 4t^3\) and \(N(t, y) = 3y^2 + 4t\), and the possible value of \(y_0\) is \(-1\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Implicit Differentiation
Implicit differentiation is a technique used when dealing with equations where the variables cannot be easily separated, which is common in many calculus problems. It involves differentiating both sides of the equation with respect to a single variable, even if the other variable appears on both sides of the equation.

In our case, the equation involves both variables, t, which is the independent variable, and y as the dependent variable. To differentiate such an implicit equation, we apply the derivative operator to each term as demonstrated in the solution. We treat y as a function of t, which implies whenever we differentiate a term with y in it, we must also incorporate y', the derivative of y with respect to t, using the chain rule.

This method reveals the underlying structure of the differential equation by clearly differentiating between the parts that vary with t and those that vary with y. It’s critical in setting up differential equations in a form that can be solved using various methods.
Initial Value Problem
An initial value problem is a type of differential equation accompanied by a specific condition that gives the value of the unknown function at a particular point. The condition, often in the form y(a) = b, is called the initial condition because it specifies where the solution begins.

Solving an initial value problem involves finding a function that not only satisfies the differential equation but also meets the stated initial condition. In the example given, we are provided with the initial condition y(0) = y_0. By substituting the initial condition into the differential equation, we can solve for y_0, thereby providing the specific solution to the initial value problem. The value y_0 is crucial because it anchors the solution curve at a known point, allowing a unique solution curve to be drawn from a family of possible solutions.
Chain Rule
The chain rule is a fundamental theorem in calculus that is used when finding the derivative of a composite function. In essence, it provides a way to differentiate a function that is 'nested' inside another. If you have a function u(g(t)), where u is a function of g, and g is a function of t, the derivative of u with respect to t is the product of the derivative of u with respect to g and the derivative of g with respect to t.

For the problem at hand, we apply the chain rule to differentiate terms like y^3, because y is a function of t. We multiply the outer derivative \(3y^2\) by the derivative of y, which is y'. This is an example of the chain rule in action, critical for handling derivatives of composite functions in differential equations.
Product Rule
The product rule is another essential concept in calculus when we need to differentiate products of two functions. According to the product rule, the derivative of a product of two functions f(t) and g(t) is given by f'(t)g(t) + f(t)g'(t). This means we take the derivative of the first function and multiply it by the second function as is, then we add the product of the first function as is with the derivative of the second function.

In our exercise, the term 4ty required the use of the product rule since it is the product of t and y. We differentiate t with respect to itself to get 1 (leaving y unchanged), and then multiply this by the derivative of y with respect to t (which is y'), and sum the two results. Correct application of the product rule helps us split the derivatives into clearly distinguishable parts, enabling the identification of functions M(t, y) and N(t, y) in exact differential equations.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

An object undergoes one-dimensional motion along the \(x\)-axis subject to the given decelerating forces. At time \(t=0\), the object's position is \(x=0\) and its velocity is \(v=v_{0}\). In each case, the decelerating force is a function of the object's position \(x(t)\) or its velocity \(v(t)\) or both. Transform the problem into one having distance \(x\) as the independent variable. Determine the position \(x_{f}\) at which the object comes to rest. (If the object does not come to rest, \(x_{f}=\infty\).) $$ m \frac{d v}{d t}=-k e^{-x} $$

In each exercise, discuss the behavior of the solution \(y(t)\) as \(t\) becomes large. Does \(\lim _{t \rightarrow \infty} y(t)\) exist? If so, what is the limit? \(y^{\prime}+y+y \cos t=1+\cos t, \quad y(0)=3\)

When modeling the action of drag chutes and parachutes, we have assumed that the chute opens instantaneously. Real devices take a short amount of time to fully open and deploy. In this exercise, we try to assess the importance of this distinction. Consider again the assumptions of Exercise 2 . A 3000 -lb dragster is moving on a straight track at a speed of \(220 \mathrm{mph}\) when, at time \(t=0\), the drag chute is opened. If we assume that the drag force is proportional to velocity and that the chute opens instantaneously, the differential equation to solve is \(m v^{\prime}=-k v\). If we assume a short deployment time to open the chute, a reasonable differential equation might be \(m v^{\prime}=-k(\tanh t) v\). Since \(\tanh (0)=0\) and \(\tanh (1) \approx 0.76\), it will take about \(1 \mathrm{sec}\) for the chute to become \(76 \%\) deployed in this model. Assume \(k=25 \mathrm{lb}-\mathrm{sec} / \mathrm{ft}\). Solve the two differential equations and determine in each case how long it takes the vehicle to slow to \(50 \mathrm{mph}\). Which time do you anticipate will be larger? (Explain.) Is the idealization of instantaneous chute deployment realistic?

A metal casting is placed in an environment maintained at a constant temperature, \(S_{0}\). Assume the temperature of the casting varies according to Newton's law of cooling. A thermal probe attached to the casting records the temperature \(\theta(t)\) listed. Use this information to determine (a) the initial temperature of the casting. (b) the temperature of the surroundings. $$\theta(t)=70+270 e^{-t}{ }^{\circ} \mathrm{F}$$

Oscillating Flow Rate A tank initially contains \(10 \mathrm{lb}\) of solvent in \(200 \mathrm{gal}\) of water. At time \(t=0\), a pulsating or oscillating flow begins. To model this flow, we assume that the input and output flow rates are both equal to \(3+\sin t \mathrm{gal} / \mathrm{min}\). Thus, the flow rate oscillates between a maximum of \(4 \mathrm{gal} / \mathrm{min}\) and a \(\mathrm{minimum}\) of \(2 \mathrm{gal} / \mathrm{min}\); it repeats its pattern every \(2 \pi \approx 6.28 \mathrm{~min}\). Assume that the inflow concentration remains constant at \(0.5 \mathrm{lb}\) of solvent per gallon. (a) Does the amount of solution in the tank, \(V\), remain constant or not? Explain. (b) Let \(Q(t)\) denote the amount of solvent (in pounds) in the tank at time \(t\) (in minutes). Explain, on the basis of physical reasoning, whether you expect the amount of solvent in the tank to approach an equilibrium value or not. In other words, do you expect \(\lim _{t \rightarrow \infty} Q(t)\) to exist and, if so, what is this limit? (c) Formulate the initial value problem to be solved. (d) Solve the initial value problem. Determine \(\lim _{t \rightarrow \infty} Q(t)\) if it exists.

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.